Vibrational Frequencies calculated at B2PLYP=FULLultrafine/6-31G*
| Mode Number |
Symmetry |
Frequency (cm-1) |
Scaled Frequency (cm-1) |
IR Intensities (km mol-1) |
Raman Act (Å4/u) |
Dep P |
Dep U |
| 1 |
A |
3606 |
3421 |
21.09 |
|
|
|
| 2 |
A |
1276 |
1211 |
0.01 |
|
|
|
| 3 |
A |
943 |
894 |
10.02 |
|
|
|
| 4 |
A |
749 |
710 |
108.62 |
|
|
|
| 5 |
A |
521 |
494 |
0.02 |
|
|
|
| 6 |
B |
3607 |
3422 |
94.88 |
|
|
|
| 7 |
B |
2238 |
2123 |
491.87 |
|
|
|
| 8 |
B |
936 |
888 |
483.28 |
|
|
|
| 9 |
B |
523 |
496 |
71.19 |
|
|
|
Unscaled Zero Point Vibrational Energy (zpe) 7198.8 cm
-1
Scaled (by 0.9487) Zero Point Vibrational Energy (zpe) 6829.5 cm
-1
See section
III.C.1 List or set vibrational scaling factors
to change the scale factors used here.
See section
III.C.2
Calculate a vibrational scaling factor for a given set of molecules
to determine the least squares best scaling factor.
Charges, Dipole, Quadrupole and Polarizability
Charges from optimized geometry at B2PLYP=FULLultrafine/6-31G*
Charges (e)
| Number |
Element |
Mulliken |
CHELPG |
AIM |
ESP |
| 1 |
C |
0.560 |
|
|
|
| 2 |
N |
-0.635 |
|
|
|
| 3 |
N |
-0.635 |
|
|
|
| 4 |
H |
0.355 |
|
|
|
| 5 |
H |
0.355 |
|
|
|
Electric dipole moments
Electric dipole components in Debye
(What's a Debye? See section
VII.A.3)
| |
x |
y |
z |
Total |
| |
0.000 |
0.000 |
2.220 |
2.220 |
| CHELPG |
|
|
|
|
| AIM |
|
|
|
|
| ESP |
|
|
|
|
Electric Quadrupole moment
Quadrupole components in D Å
| Primitive |
| | x | y | z |
| x |
-16.541 |
4.340 |
0.000 |
| y |
4.340 |
-16.046 |
0.000 |
| z |
0.000 |
0.000 |
-17.128 |
|
| Traceless |
| | x | y | z |
| x |
0.046 |
4.340 |
0.000 |
| y |
4.340 |
0.788 |
0.000 |
| z |
0.000 |
0.000 |
-0.834 |
|
| Polar |
| 3z2-r2 | -1.669 |
| x2-y2 | -0.495 |
| xy | 4.340 |
| xz | 0.000 |
| yz | 0.000 |
|
Polarizabilities
Components of the polarizability tensor.
Units are
Å
3 (Angstrom cubed)
Change units.
| |
x |
y |
z |
| x |
1.799 |
0.390 |
0.000 |
| y |
0.390 |
6.035 |
0.000 |
| z |
0.000 |
0.000 |
1.776 |
<r2> (average value of r
2) Å
2
| <r2> |
39.060 |
| (<r2>)1/2 |
6.250 |